Notice Of Cancellation

NOTICE OF CANCELLATION

INCH-POUND MIL-STD-285 NOTICE 1 24 October 1997

MILITARY STANDARD Attenuation Measurements for Enclosures, Electromagnetic Shielding, For Electronic Test Purposes, Method Of

MIL-STD-285, dated 25 June 1956, is hereby canceled. The preparing activity for this document has determined that IEEE-STD-299 is a suitable replacement for this standard. Users are cautioned to evaluate this document for their particular application before citing it as a replacement document. (Applications for copies of IEEE publications should be addressed to Institute of Electrical and Electronics Engineers, IEEE Service Center, 445 Hoes Lane, P.O. Box 1331, Piscataway, NJ 08855.)

Custodian: Army - CR Navy - EC

Preparing Activity: Army - CR (Project EMCS-0167)

AMSC N/A

AREA EMCS

DISTRIBUTION STATEMENT A. Approved for public release; distribution is unlimited.

MIL-STD-285 25 June 1956 SUPERSEDING MIL-A-18123(SHIPS) 1 August 1954 MILITARY STANDARD ATTENUATION MEASUREMENTS FOR ENCLOSURES, ELECTROMAGNETIC SHIELDING, FOR ELECTRONIC TEST PURPOSES, METHOD OF UNITED STATES GOVERNMENT PRINTING OFFICE WASHINGTON: 1956 ÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄÄ For sale by the Superintendent of Documents, U.S. Government Printing Office, Washington 25, D.C., Price 15 cents

MIL-STD-285 25 June 1956 OFFICE OF THE ASSISTANT SECRETARY OF DEFENSE WASHINGTON 25, D.C. Supply and Logistics

25 June 1956

ATTENUATION MEASUREMENTS FOR ENCLOSURES, ELECTROMAGNETIC SHIELDING, FOR ELECTRONIC TEST PURPOSES, METHOD OF MIL-STD-285 1. This standard has been approved by the Department of Defense and is mandatory for use of the Departments of the Army, the Navy, and the Air Force. 2. In accordance with established procedure, the Standardization Division has designated the Signal Corps, the Bureau of Ships, and the Air Force, respectively, as Army-Navy-Air Force custodians of this standard. 3. This standard is mandatory for use effective 25 June 1956 by the Departments of the Army, the Navy, and the Air Force. 4. Recommended corrections, additions, or deletions should be addressed to the Standardization Division, Office of the Assistant Secretary of Defense (Supply and Logistics), Washington 25, D.C.

MIL-STD-285 25 June 1956 CONTENTS 1.

SCOPE

2.

APPLICABLE DOCUMENTS

3.

DEFINITIONS

3.1

Attenuation

3.2

Voltage versus power ratio

4.

REQUIREMENTS

4.1

Test set-up

4.1.1

Measurement of attenuation of low impedance (magnetic) fields

4.1.2

Measurement of attenuation to high impedance (electric) fields

4.1.3

Measurement of attenuation to plane waves Figures

1.

Attenuation measurement low impedance magnetic field

2.

Source of intense peak power magnetic field

3.

Attenuation measurement high impedance electric field

4.

Source for intense peak power electric field

5.

Attenuation test for plane waves (wave impedance = 377 ohms)

6.

Signal source for plane waves at 400 mc.

MIL-STD-285 25 June 1956 ATTENUATION MEASUREMENTS FOR ENCLOSURES, ELECTROMAGNETIC SHEILDING, FOR ELECTRONIC TEST PURPOSES, METHOD OF 1.

SCOPE

1.1 This standard covers a method of measuring the attenuation characteristics of electromagnetic shielding enclosures used for electronic test purposes over the frequency range 100 kilocycles to 10,000 megacycles. 2.

APPLICABLE DOCUMENTS

3.

DEFINITIONS

3.1 Attenuation.--Attenuation is the ratio, expressed in decibels (db), of the received powers on opposite sides of a shield when the shield is illuminated by electromagnetic radiation; and as used in this standard, is the figure of merit to designate the shielding effectiveness of electromagnetic enclosures. 3.2 Voltage versus power ratio.--In accordance with 3.1, measurement should be made of powers associated with the incident wave, and the ratio of these measurements should be expressed in decibels. It is acceptable instead, when the wave impedance is identical for EÚ1¿ and EÚ2¿ to measure only the electric field intensities, EÚ1¿ and EÚ2¿ and to use the expression: EÚ1¿ Attenuation (db)=20 log ÄÄÄÄ EÚ2¿ It is assumed that the wave impedance will be identical and that this method is used for the sake of convenience. 4.

REQUIREMENTS

4.1 Test set-up.--The arrangement of signal sources, measuring equipments, pick-up devices, and shielded enclosures shall be in accordance with the following paragraphs and figures 1 through 6. All power lines, RF cables, and other utilities entering the shielded enclosure shall be in place when tests are conducted. Special care shall be taken to make measurements in the vicinity of utility entrances, doors, and access panels. 4.1.1

Measurement of attenuation low impedance (magnetic) fields.

4.1.1.1 Attenuator.--When an attenuator, the calibration of which is used as a basis for the desired measurements, is employed between either the receiver or the transmitter and its antenna, the antenna shall "look back" into an impedance which is independent of the setting of the attenuator. The attenuator A may be a 50 or 72 ohm transmission line, low input impedance, step attenuator. A signal generator shall be used to calibrate the attenuator. The attenuator shall be capable of measuring an insertion loss of over 70 db. 4.1.1.2 Detector.--The detector may be any the BC-348-Q or a field strength meter provided such as the Radio Test Set AN/PRM-1, AN/PRM-14, Incorporated, NF-114. A matching device may be

receiver such as the DZ-2 or with a low impedance input and Empire Devices, used with high input

impedance receivers or field strength meters. 4.1.1.3

Signal source.

4.1.1.3.1 Signal source S may be a signal generator or power oscillator of sufficient CW, MCW or Pulsed CW output. In case loop LÚ1¿ is connected to the output of a signal generator 1

MIL-STD-285 25 June 1956 or power oscillator, a tuning capacitor may be connected in series with LÚ1¿ to obtain resonance at the test frequency used. 4.1.1.3.2 If the signal generator has a reliable output attenuator, it may be used, instead of the attenuator A, to obtain an equivalent ratio of EÚ1¿/EÚ2¿ for the calculation of the attenuation of the shielding enclosure by using the detector D at the same reference level when the shielding enclosure wall is removed. In this case, no precaution has to be taken to guard against case leakage at the detector. 4.1.1.3.3

A signal source shall be constructed as shown on figure 2.

4.1.1.4 Measurement of db attenuation.--Measurement of db attenuation to low impedance magnetic fields shall be performed in accordance with figure 1. 4.1.1.4.1 The attenuation of the enclosure is the increase in the db setting of the attenuator A necessary to obtain the same reference reading level in detector D, when the shielding enclosure wall, SÚ1¿ SÚ2¿ is removed, without changing the relative positions of LÚ1¿ and LÚ2¿. (The attenuation in db is also essentially equal to 20 log EÚ1¿/EÚ2¿, where EÚ2¿and EÚ1¿ are the voltages induced in the receiving loop, with the enclosure wall in and with the enclosure wall removed, respectively, without changing the relative positions of LÚ1¿ and LÚ2¿.) The equipment as a whole shall be capable of measuring a shielded enclosure attenuation of at least 100 db. 4.1.1.4.2 The position of LÚ1¿ with respect to the enclosure shall be anywhere around the enclosure and in any orientation to the section seams and access panel seams. A reading shall be taken on all four sides of the enclosure, and the minimum attenuation recorded. This shall be a minimum of 70 db. 4.1.1.4.3 When it becomes impractical to remove the shielding enclosure wall SÚ1¿, SÚ2¿, the loops LÚ1¿ and LÚ2¿ shall be set outside the enclosure in an exactly similar position with no obstruction. Because the strong magnetic field generated by LÚ1¿ can penetrate the metal case of detector D and attenuator A, these two equipments shall be left inside the enclosure and the loop LÚ2¿ brought out of the enclosure through a transmission line connector. The connector shall be grounded circumferentially where it passes through each wall of the shielded enclosure. Shielded enclosure doors shall be closed during tests. 4.1.1.4.4 A test shall be made to insure that no case leakage exists at D and A. The detector should show no indication whatever above the inherent background when cable CÚ2¿ or CÚ3¿ is disconnected. 4.1.2 Measurement of attenuation to high impedance (electric) fields (see figure 3). 4.1.2.1 Attenuator.--The attenuator used may be a high impedance capacity type attenuator, similar to the external attenuator used with the Ferris Model 32A(TS-432/U) or constructed similarly to the one used internally on the AN/PRM-1. A signal generator shall be used to calibrate this attenuator. The attenuator shall be able to measure an insertion loss of over 100 db. 4.1.2.2 Detector.--The detector may be a field strength meter such as the Ferris 32A(TS-432/U), the AN/PRM-1, the AN/PRM-14, and Empire Devices, Incorporated, NF-114. In this case, attenuator A may be deleted as these

instruments can measure induced voltages in the receiving antenna RÚ2¿, and are able to record levels 100 db apart. The readings obtained on these instruments shall be checked against a signal generator. 4.1.2.2.1 When the receiver is used as other than a fixed reference level indicator, and the signal source is a broadband device such as described on figures 2 and 4, the output indication of the receiver shall drop at ]east 30 db: (a) when the local oscillator is disabled, (b) while in the strongest field, and (c) at the highest input level to the first tube to be used during the test of the shielded enclosure. Also, the image rejection shall be at least 30 db, and the IF rejection shall be at least 40 db, when broad band signals are used. The case leakage and power-line filtering of the receiver-attenuator combination shall be such that when 2

MIL-STD-285 25 June 1956 operating in the strongest field required to he measured, removing the antenna and substituting a shielded dummy antenna simulating the actual antenna impedance will result in at least a 30 db reduction of output indication. 4.1.2.3 A receiver such as the BC-348-Q may be used. In this case, they are used only as reference level indicators. The attenuation may be read on attenuator A. The equal reference level chosen shall be low enough as not to represent any overloading or saturation of the receiver. If necessary, a matching device may be used with low input impedance receivers. 4.1.2.4

Signal source.

4.1.2.4.1 Signal source S may be a signal generator or power oscillator of sufficient CW, MCW or pulsed CW output. The termination of cable CÚ1¿ may be matched to the signal source S if desired. 4.1.2.4.2 If the signal generator has a reliable output attenuator, it may be used instead of the attenuator A, to obtain an equivalent ratio of EÚ1¿/EÚ2¿ for the calculation of the db attenuation of the enclosure by operating the detector D at the same reference level when the shielding enclosure wall is removed. In this case, no precaution has to be taken to guard against case leakage at the detector. 4.1.2.4.3 If a large output signal generator or power oscillator is not available, a pulse signal source may be easily constructed as shown on the three set-ups on figure 4. 4.1.2.5

Measurement of db attenuation, (see figure 3).

4.1.2.5.1 The attenuation of the enclosure is the increase in the db setting of the attenuator A necessary to obtain the same reference reading level in detector D when the shielding enclosure wall SÚ1¿ and SÚ2¿ is removed, without changing the relative position of RÚ1¿ and RÚ2¿. The attenuation in db is also essentially equal to 20 log 10 EÚ1¿/EÚ2¿, where EÚ2¿ and EÚ1¿ are the voltages induced in receiving rod with the enclosure wall in and with the enclosure wall removed, respectively. 4.1.2.5.2 The positioning of RÚ1¿ with respect to the shielding enclosure walls shall be any where around the enclosure, in any orientation to the section seams and access-panel seams. A reading shall be taken at each side of the shielding enclosure and the minimum attenuation recorded. This minimum shall be over 100 db. 4.1.2.5.3 When it becomes impractical to remove the shielding enclosure walls, SÚ1¿ and SÚ2¿, both rods RÚ1¿ and RÚ2¿ shall he set outside the enclosure in the exact similar position, with no obstruction. Because the strong electric fields generated by RÚ1¿ can penetrate the metal case of detector D and attenuator A, theme two equipments shall be left inside the enclosure and the rod RÚ2¿ brought out of the enclosure through a transmission line connector. The cable used shall be as short as possible. The connector shall be grounded circumferentially where it passes through each wall of the shielded enclosure. Shielded enclosure doors shall be closed during the test. 4.1.2.5.4 A test shall be made to ensure that no case leakage exists at D or A. The detector should show no indication whatsoever above inherent background when cable CÚ2¿ or CÚ3¿ is disconnected.

4.1.3

Measurement of attenuation to plane waves (see figure 5).

4.1.3.1

Attenuator.--The attenuator shall be as specified in 4.1.1.1.

4.1.3.2 Detector.--The detector may be a receiver such as Receiving Equipment AN/APR 4, RF Interference Test Set AN/URM-28, RF Interference Test Set AN/URM-29, Radio Set AN/ARC-7, or a field strength meter such as the Noise Field Intensity Meter TS-587/U, Radio Test Set AN/URM-17, AN/URM-7 or Empire Devices, Incorporated, NF-105. Detectors which cannot readily give peak indications may he used with an oscilloscope connected to their output. 4.1.3.3

Signal source.

4.1.3.3.1 Signal source S may be a signal generator or power oscillator of sufficient CW, 3

MIL-STD-285 25 June 1956 MCW, or pulsed CW output. The terminal of cable CÚ1¿ may be matched to the signal source when necessary. 4.1.3.3.2 If the signal generator has a reliable output attenuator, it may be used instead of attenuator A, to obtain an equivalent ratio of EÚ1¿/EÚ2¿ for the calculation of the attenuation of the enclosure by using the detector D at the same reference level. In this case, no precaution may have to be taken to guard against leakage at the detector. 4.1.3.3.3 The signal source may be an AN/ARC-27 transmitter, a high frequency Rollin Signal generator Model 30(TS608/U), or equal, or Radar Set AN/APT-5 radar transmitter. An oscillator, tuned to the frequency of test may be constructed, using a high voltage plate supply and then pulsed, to obtain high peak power. A signal source may be constructed as shown on figure 6. 4.1.3.4

Measurement of db attenuation (see figure 5).

4.1.3.4.1 The attenuation of the enclosure in db is equal to the increase in the db setting of attenuator A necessary to obtain the same reference reading level in detector D when the receiving antenna is switched from position RÚ2¿ to RÚ3¿, without changing the position of RÚ1¿. (The attenuation in db is also essentially equal to 20 log 10 EÚ1¿/EÚ2¿, where EÚ1¿/EÚ2¿ are the voltages induced in RÚ3¿ and RÚ2¿, respectively.) 4.1.3.4.2 walls shall be to the section taken, and the db.

The position of RÚ1¿ with respect to the shielding enclosure anywhere around the enclosure in any orientation with respect seams and access-panel seams. Several readings shall be minimum attenuation recorded. This minimum shall be over 100

4.1.3.4.3 A test shall be made to insure that no case leakage exists at D or A. The detector D should show no indication whatsoever above inherent background when cable CÚ2¿ or CÚ3¿ is disconnected. Copies of specifications, standards, drawings, and publications required by contractors in connection with specific procurement functions should be obtained from the procuring agency or as directed by the contracting officer. Copies of this standard for military use may be obtained as indicated in the forward to the index of Military Specifications and Standards. Copies of this standard may be obtained for other than official use by individuals, firms, and contractors from the Superintendent of Documents, U.S. Government Printing Office, Washington 25, D.C. Both the title and identifying symbol number should be stipulated when requesting copies of military standards. Custodians: Army--Signal Corps Navy--Bureau of Ships Air Force Other interest: Army--O Navy--Or

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